Proof in multi-variable functions

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I am facing this question and can't get my head around where to start. I have tried a couple of things. let $r=\sqrt{x^2+y^2+z^2}$ and $u=f(r)$, and $f_{xx} + f_{yy}+f_{zz}=0$. Then prove that there exists $a$,$b$ $\in \mathbb{R}$ where $f(r)=\frac{a}{r}+b$. I know the rules say that you should write some stuff about the things you have tried, but I can't wrap my head around where to start.

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The question is a bit unclear, but you are essentially asking for solutions of Laplace's equation, $\nabla^2 U=0$, in spherical coordinates. And yes, it so happens that $U(r,\theta,\phi)=\frac{a}{r}+b ~$ is a particular (but not general) solution. This comes from the fact that the scalar Laplacian is $$\nabla^2 U(r,\theta,\phi)=\frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2\frac{\partial U}{\partial r}\right)+\frac{1}{r^2\sin^2(\phi)}\frac{\partial^2 U}{\partial \theta^2}+\frac{1}{r^2\sin(\phi)}\frac{\partial}{\partial \phi}\left(\sin(\phi)\frac{\partial U}{\partial \phi}\right).$$ Assuming no $\theta$ or $\phi$ dependence this can be reduced to $$\nabla^2 U(r)=\frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2\frac{\partial U}{\partial r}\right)=0.$$ We notice that a constant function $U(r)=b$ works. Multiplying both sides by $r^2$, $$\frac{\partial}{\partial r}\left(r^2\frac{\partial U}{\partial r}\right)=0$$ $$r^2\frac{\partial U}{\partial r}=A$$ $$\frac{\partial U}{\partial r}=\frac{A}{r^2}\implies U(r)=\frac{-A}{r}=\frac{a}{r}.$$ We have found two linearly independent solutions, and since this ODE is of second order, these must be the only two solutions. Thus the "general" solution is a linear combination: $$U(r)=\frac{a}{r}+b.$$